Deriving Average Energy Function For A Classical DOF

In summary, the conversation revolves around the question of why integration is done between 0 and infinity when dealing with the absolute value of c. It is explained that negative values of c are not considered because the absolute value will cancel out the integration. The importance of including the absolute value is also mentioned, as it affects the result of the integral.
  • #1
Bashyboy
1,421
5
Hello everyone,

The problem I am currently working is exactly what is given in this link: https://www.physicsforums.com/showthread.php?t=554243

However, I do not understand why we integrate between 0 and infinity. What is the motivation for doing so?
 
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  • #2
It's because of the absolute value of c. You have no reason to consider negative c's, since the absolute value will cancel the integration.
 
  • #3
Do you perhaps mean the absolute value of q?
 
  • #4
Yes.
The result Steve writes blows up at minus infinity (if c>0), so the integral is not 0 at all: it doesn't exist.
That's because he omitted the | | .
E = c |q| can be integrated. From minus infinity to 0 is exactly the same as from 0 to infinity.
 
  • #5


Hello,

The motivation for integrating between 0 and infinity in this case is to account for all possible energies that the classical degree of freedom (DOF) can have. By integrating from 0 to infinity, we are considering all possible values of energy, from the lowest possible value (0) to the highest possible value (infinity). This allows us to accurately calculate the average energy of the DOF, as it takes into account the entire range of possible energies. Additionally, integrating from 0 to infinity is a common approach in classical mechanics and statistical mechanics, as it allows us to consider all possible states of a system. I hope this helps clarify the reasoning behind this approach.
 

Related to Deriving Average Energy Function For A Classical DOF

What is a classical degree of freedom (DOF)?

A classical degree of freedom (DOF) refers to a specific type of movement or vibration that a molecule or particle can have in a system. In classical mechanics, these DOFs are described using Newton's laws of motion and can include translational, rotational, and vibrational motions.

What is the importance of deriving an average energy function for a classical DOF?

Deriving an average energy function for a classical DOF allows us to understand and predict the behavior of a system at a macroscopic level. By understanding the average energy of a DOF, we can accurately describe the thermodynamic properties of a system and make predictions about its behavior.

What is the mathematical process for deriving an average energy function for a classical DOF?

The mathematical process for deriving an average energy function for a classical DOF involves using statistical mechanics and the Boltzmann distribution to calculate the average energy of a system. This involves integrating over all possible states of the system and taking into account the probabilities of each state occurring.

How does temperature affect the average energy function for a classical DOF?

Temperature plays a crucial role in the average energy function for a classical DOF. As temperature increases, the average energy of a DOF also increases. This is because at higher temperatures, there is more thermal energy available to drive the motion and vibrations of the molecules or particles in the system.

What are some real-world applications of deriving average energy functions for classical DOFs?

The average energy function for classical DOFs has many real-world applications, including in the fields of thermodynamics, chemical kinetics, and materials science. It is used to understand the behavior of gases, liquids, and solids, and is crucial in the design and development of new materials and chemical reactions.

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